1. 4/8/2015PHY 752 Spring 2015 -- Lecture 291 PHY 752 Solid State Physics 11-11:50 AM MWF Olin 107 Plan for Lecture 29:  Chap. 22 in Marder & pdf file on “Maximally Localized Wannier Functions”  Electromagnetic properties of insulators  Modern theory of polarization

2. 4/8/2015PHY 752 Spring 2015 -- Lecture 292

3. 4/8/2015PHY 752 Spring 2015 -- Lecture 293

4. 4/8/2015PHY 752 Spring 2015 -- Lecture 294 Electromagnetic properties of insulating materials Some references: “Maximally localized Wannier functions: Theory and applications”, Marzari et al., RMP 84, 1419 (2012) “Macroscopic polarization in crystalline dielectrics: the geometric phase approach”, Resta, RMP 66, 899 (1994) “Electric polarization as a bulk quantity and its relation to surface charge”, Vanderbilt and King-Smith, PRB 48, 4442 (1993)

5. 4/8/2015PHY 752 Spring 2015 -- Lecture 295

6. 4/8/2015PHY 752 Spring 2015 -- Lecture 296 Notion of an electric dipole moment summing over eigenstates of the system  ”Modern” theory of polarization can be formulated in terms of Wannier functions or in terms a Berry- phase expression. All of the formulations define the polarization modulo eR/V, where R is a lattice translation and V is the volume of the unit cell.

7. 4/8/2015PHY 752 Spring 2015 -- Lecture 297 Ambiguity of polarization P1P1 P2P2

8. 4/8/2015PHY 752 Spring 2015 -- Lecture 298 Notion of Wannier functions formed from Bloch eigenstates:

9. 4/8/2015PHY 752 Spring 2015 -- Lecture 299 Construction of Wannier function from Bloch states Inverse transform: Non-uniqueness of Wannier functions; suppose a Bloch function is multiplied by an arbitrary phase:  constructed Wannier function would change

10. 4/8/2015PHY 752 Spring 2015 -- Lecture 2910 Simple example of Wannier function

11. 4/8/2015PHY 752 Spring 2015 -- Lecture 2911 In addition to the arbitrary phase problem, it is often the case that there are multiple or entangled bands needed to form the Wannier states.  Turning problem into an advantage – notion of maximally localized Wannier functions

12. 4/8/2015PHY 752 Spring 2015 -- Lecture 2912 Some details: Normalization of Bloch waves: Orthogonality of Wannier functions:

13. 4/8/2015PHY 752 Spring 2015 -- Lecture 2913 Notion of maximally localized Wannier function is to use the non-uniqueness to choose the phase in order to maximize the localization of the Wannier function

14. 4/8/2015PHY 752 Spring 2015 -- Lecture 2914 Practical calculation of localization function Actually these expressions must be evaluated using finite differences in k. The localization function is minimized by means of a unitary transformation on the phase of the Bloch functions:

15. 4/8/2015PHY 752 Spring 2015 -- Lecture 2915 Some examplesGraphene

16. 4/8/2015PHY 752 Spring 2015 -- Lecture 2916 Wannier functions used to evaluate polarization Wannier function in central cell:

17. 4/8/2015PHY 752 Spring 2015 -- Lecture 2917 Polarization of system depends on position weighted sum of both electronic charges and on ionic charges:

18. 4/8/2015PHY 752 Spring 2015 -- Lecture 2918

19. 4/8/2015PHY 752 Spring 2015 -- Lecture 2919 Note that we previously noticed that the Bloch functions and the corresponding Wannier functions are not unique, but we can shown that r n is unique up to a lattice translation (thanks to Vanderbilt and King-Smith) We assume the Bloch waves have the symmetry: Consider the transformed Bloch wave:

20. 4/8/2015PHY 752 Spring 2015 -- Lecture 2920

21. 4/8/2015PHY 752 Spring 2015 -- Lecture 2921 Vanderbilt and King-Smith note that with this definition of the polarization, the surface charge of a polar material is consistent with